bobc2 said:
ghwellsjr: I have never used the term "hyperplanes of simultaneity" so now I guess I have to try to figure out what you mean by the term. If you go back to post #9 and look at the three graphs representing three different IRF's, each one of them is showing just one spatial dimension because, as is common in spacetime diagrams, we use the other dimension for time and we limit the activity in the scenario to just one dimension (usually referred to as the x-dimension) and we assume that the audience is familiar enough with this type of diagram that they know that the y- and z-dimensions are not shown but since nothing is happening at locations other than y=0 and z=0, we mentally recognize that when the graph shows a horizontal grid line, that is a line of simultaneity for a particular value of time which you look up at the left side of the graph and it means that all events along that horizontal line are simultaneous meaning they happen at the same time in that IRF. (I can't believe I'm explaining all this--nevertheless, I carry on.) Now since we don't show the y- and z- dimensions, we mentally realize that all the events that are simultaneous along that line are extrapolated out in those two extra dimensions so it is really a volume of simultaneity which I suppose is identical to your term hyperplane of simultaneity.
Bobc2: Yes, we are on the same page here. Actually you do find the term “hyperplanes of simultaneity" in many places in the special relativity literature—and you have correctly figured out its meaning. I’m glad we have no problem reducing the analysis to the use of just two dimensions in our sketches.
But let's make it very clear that it's one dimension of space and one dimension of time. It's a 1-D scenario, agreed?
bobc2 said:
ghwellsjr: Now what's important is that two (or more) events that are simultaneous in one IRF (because they have the same value for their time coordinate) may not be simultaneous in another IRF as can be seen if you look at the three different graphs. I never really stopped to think in terms of a volume of simultaneity, assuming that that is what you mean by a hyperplane of simultaneity, but it is obviously the case although I would say it is so obvious that it doesn't need to be said.
Bobc2: Yes, we are in perfect agreement on that. And when I use the term "hyperplanes of simultaneity" I also don't see a need to show all dimensions in the space-time diagrams.
ghwellsjr: Now if we wanted to show a two-dimensional scenario where the observers were moving around in both the x- and y-dimensions, we'd have a hard time putting that on a piece of paper…
Bobc2: But, that’s just what I’ve been trying to do with the space-time diagrams that include the various X1 axes for the different observers as well as the X4 axes. These axes are of course all identified using the velocities of the moving observers along with the Lorentz transformation. (see my first sketch below)
Now maybe you can see why I made my previous comment. When I talk about a 2-D scenario, I specifically said two spatial dimensions, not one of space and one of time. I have never seen any of your diagrams that include anything more than X1 and X4. X4 is always the time dimension, correct? All your diagrams are for a 1-D scenario, not a 2-D scenario, agreed?
bobc2 said:
ghwellsjr: …but what we could do with today's technology is make an animation and present it as a movie. Each frame of the movie marks out a plane of simultaneity but the assumption is that it extends out into the z-dimension and so there really is a volume of simultaneity. Does that communicate? Does it make sense to you? Is it in agreement with your concept of the hyperplane of simultaneity?.
Bobc2: Yes, it certainly does. I have among my special relativity computer files examples of such an animation. And I’ve seen one posted on our forum here.
And would that be one that I
posted?
bobc2 said:
So, the sketch below illustrates how I show two different hyperplanes of simultaneity, blue and red, where two different observers are moving at the same speed in opposite directions with respect to the black inertial reference frame (the perpendicular coordinates representing X1 and X4 axes).
I have included the representation of a rod moving to the right with respect to the black frame, but the rod is at rest in the blue inertial frame. Thus, we see directly the length contraction aspect of special relativity. Blue sees the length of the rod as L0, whereas Red sees the rod length as L. And the reason I've used the symmetric space-time diagram (first introduced by Loedel of Mexico who received Einstein's blessing during their visit), is that it avoids the need to worry about the meaning of the line distances when comparing Blue and Red coordinates (you don't really need to be concerned with the hyperbolic calibration curves). This scheme was introduced to me in my first grad school special relativity course. My prof was fond of this means of communicating special relativity. I used it also later on when I was a physics instructor for undergrad physics and engineering students.
Here's where my eyes glaze over. I'm not saying that there is anything wrong with your diagrams, I don't know, because I'm not motivated to learn about them. I don't see the attraction for them. They don't communicate anything that can't be communicated in a series of simple graphs like the ones I presented in post #9. Do you think they communicate something more than several IRF type graphs?
bobc2 said:
Of course it is easy to account for both X1 and X4 coordinates of Blue and Red using the Lorentz transformation hyperbolic calibration curves as shown below (the Red and Blue colors are reversed from the above sketch).
Maybe it's easy for you but not for me.
I can understand how these kinds of graphs would be important a hundred years ago but nowadays, we can let our computers take care of all the computations.
bobc2 said:
I was just trying to see if we are on the same page about the significance of these two different 3-D worlds (represented within the 4-dimensional space with just two coordinates) that blue and red occupy at points along their respective worldlines.
We probably aren't on the same page, especially if you see eye-to-eye with Vandam, because he thinks the three separate IRF plots hide or mask information that is evident on the kinds of diagrams you make. Do you share his opinion?
I don't hand-draw my plots. I use a computer and once I set up a scenario, the computer draws the first plot in the same IRF that I entered the scenario into. Then I enter a speed parameter that creates a new plot using the Lorentz Transformation. I repeat for the third plot. So I know that there is no more information in the second and third plots (or as many others as I want to make) than there is in the first one.
My question to you is: would it be possible to have a computer take the scenario the way I set it up for the first IRF and then instead of transforming to an IRF at a different speed, could it generate one of your diagrams that combines the information from three simple IRF graphs?
There is one piece of information that can be gleaned from watching the computer redraw the graphs for the different IRF's that you would not see from anyone of them and that is it makes it obvious which characteristics are frame invariant and which are not but aside from that, no new insight or conclusions can be obtained simply by presenting the same information in different IRF's or in one of your (or Vandam's) diagrams that combine the information from multiple IRF's. Do you agree with this assessment?
bobc2 said:
Finally, here is an interesting sketch, using the above concepts of hyperplanes of simultaneity to illustrate the motivation for the Block Universe model of special relativity. For now, I will spare you the pain of the addition of world lines of many different laser pulses (idealized in the diagrams as single photons). So, there is a scheme for deciphering the many laser light measurements that could be performed on signals transmitting back and forth and intersecting along the different world lines. To make the measurements more convincing you just add more observers at rest in the Blue inertial frame (collaborating results with any amount of data desired), and have matching Red observers participating in the experiment.
My hat's off to anyone that can make sense out of these diagrams, let alone, draw them.
bobc2 said:
Perhaps I have not communicated these concepts well, or perhaps you understand the concept quite well and simply reject it. I just wanted to make sure I understood your thinking on these hyperplanes of simultaneity (X2 and X3 coordinates suppressed for clarity)
If by "concept", you mean your diagrams, then you can fault the student--not the teacher. But if you mean, as you posed the question to me earlier, the concept of simultaneity, then I understand it quite well. It's simply all the events that have the same time coordinate in any given IRF.
bobc2 said:
Maybe my basic questions are:
1) Do you accept the validity of the above sketches as correctly representing key aspects of special relativity (regardless of whether you attach any physical significance to it)?
Since others accept their validity, then I will accept their opinion.
Do you accept the validity of graphs like the ones on page #9 as being exactly equivalent to your diagrams?
bobc2 said:
2) Do you attach any physical significance to these hyperplanes of simultaneity?
No, not in your diagrams or in the type that I draw.
Do you attach any physical significance to the origin of an IRF?
bobc2 said:
3) What significance at all to the hyperplanes of simultaneity represented in the above space-time diagrams.
IRF's are man-made constructs. If they exist physically in nature, we have no way of determining that. It's like asking for the absolute rest state of the ether. Even we believe, like Lorentz that such an ether exists, we still would prefer Einstein's Special Relativity over a Lorentz Ether Theory because the Transformation process allows us to make any IRF just as valid as the one and only ether IRF.
All of Special Relativity, not just issues of simultaneity are very important in our understanding of the world. Without it, we would still be floundering around searching for that illusive ether. Without it, we would not have the simple and consistent means of interpreting the data from our measurements. One of the most important tenets of SR is that there is no preferred reference frame. It appears to me that you and Vandam want to get rid of all reference frames in favor of some super interpretation that incorporates several reference frames all at the same time. One of the other important tenets of SR is that you don't conflate coordinates from two or more reference frames which is what I see you and Vandam doing.
One last question: what does any of this have to do with the issue of whether time dilation is observable or measurable by the observers in the scenario?